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Inclusive and Semiinclusive $\rho^0$ Production in $\pi^+ / \pi^- / K^+ / P P$ Interactions at 147-{GeV}/$c$

Schouten, M. ; De Bock, H. ; Dziembowski, Z. ; et al.

Z.Phys.C 9 (1981) 93-104, 1981.

Inspire Record 170594 DOI 10.17182/hepdata.1419

In an experiment with the 30-inch Hybrid Spectrometer at Fermilab we have obtained the inclusive and semi-inclusive production cross sections of the ϱ0 meson using a conventional background subtraction technique. Production cross sections for the ϱ0 are derived as a function of the Feynman scaling variablex, and the transverse variablespt2 andEt=(pt2+M2)1/2. The longitudinal distributions are compared with the (1−x) dependence of the proton and meson valence quark structure functions, using various forms of recombination and fragmentation models. The transverse distributions are compared with thermodynamic models. We give density matrix elements for the ϱ0 production from pions in the extreme forward region.

6 data tables

Table 1

No description provided.

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Table 3

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Diffraction Processes in $\pi^- p$ Interactions at $p=40$-{GeV}/$c$

Grishin, V.G. ; Kanarek, T. ; Kvatadze, R.A. ; et al.

Sov.J.Nucl.Phys. 35 (1982) 215, 1982.

Inspire Record 167728 DOI 10.17182/hepdata.18757

None

6 data tables

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INCLUSIVE PRODUCTION OF MESON RESONANCES IN MULTI - NUCLEON INTERACTIONS OF pi- MESONS WITH CARBON NUCLEI AT P = 40-GeV/c

Grishin, V.G. ; Kvatadze, R.A. ; Simic, L. ;

Sov.J.Nucl.Phys. 34 (1981) 703, 1981.

Inspire Record 164804 DOI 10.17182/hepdata.39157

None

4 data tables

Table 1

No description provided.

Table 2

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Table 3

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The Effective Energy Dependence of the Charged Particle's Multiplicity in $P / \pi^+ / K^+$ Interactions on Protons at 147 GeV/c

Brick, D. ; Rudnicka, H. ; Shapiro, A.M. ; et al.

Phys.Lett.B 103 (1981) 241-246, 1981.

Inspire Record 170358 DOI 10.17182/hepdata.6707

The energy dependence of the average of the charged multiplicity and its dispersion in π + /K + /p interaction on protons at 147 GeV/ c is found to be the same as in e + e − annihilations if an “effective energy” variable is used instead of the total energy. The effective energy S eff is defined as the invariant mass of all secondaries left after the two leading particles have been removed. Fitting the expression aS eff b to the average charge multiplicity 〈 n ch 〉, we find the power b to be in good agreement with the value of 0.25 predicted by Fermi's statistical model and by Landau's hydrodynamical model.

6 data tables

Table 1

BINS IN WEFF SELECTED SO AS TO YIELD 200 EVENTS IN EACH BIN.

Table 2

200 EVENTS IN EACH BIN IN WEFF.

Table 3

50 EVENTS IN EACH BIN IN WEFF.